Electrical properties and structure of p-type amorphous oxide semiconductor xZnO•Rh2O3

被引:51
作者
Kamiya, T
Narushima, S
Mizoguchi, H
Shimizu, K
Ueda, K
Ohta, H
Hirano, M
Hosono, H
机构
[1] Tokyo Inst Technol, Mat & Struct Lab, Midori Ku, Kanagawa 2268503, Japan
[2] Keio Univ, Dept Econ, Minato Kita Ku, Yokohama, Kanagawa 2238521, Japan
[3] Tokyo Inst Technol, Frontier Collaborat Res Ctr, JST, ERATO,SORST,Midori Ku, Yokohama, Kanagawa 2268503, Japan
[4] Kyushu Inst Technol, Tobata Ku, Fukuoka 8048550, Japan
[5] Nagoya Univ, Chigusa Ku, Nagoya, Aichi 4648603, Japan
关键词
D O I
10.1002/adfm.200400046
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
p-Type conduction in amorphous oxide was firstly found in zinc rhodium oxide (ZnO-Rh2O3) (Adv. Mater 2003,15,1409), and it is still the only p-type amorphous oxide to date. It was reported that an ordered structure at the nanometer scale was contained and its electronic structure is not clear yet. In this paper, optoelectronic and structural properties are reported in detail for xZnO center dot Rh2O3 thin films (x = 0.5-2.0) in relation to the chemical composition x. All the films exhibit positive Seebeck coefficients, confirming p-type conduction. Local network structure strongly depends on the chemical composition. Transmission electron microscopic observations reveal that lattice-like structures made of edge-sharing RhO6 network exist in 2-3 nm sized grains for rhodium-rich films (x = 0.5 and 1.0), while the zinc-rich film (x = 2) is completely amorphous. This result indicates that excess Zn assists to form an amorphous network in the ZnO-Rh2O3 system since Zn ions tend to form corner-sharing networks. The electronic structure of an all-amorphous oxide p-ZnO center dot Rh2O3/n-InGaZnO4 junction is discussed with reference to electrical characteristics and results of photoelectron emission measurements, suggesting that the p/n junction has large band offsets at the conduction and valence bands, respectively.
引用
收藏
页码:968 / 974
页数:7
相关论文
共 33 条
[1]   MECHANISM OF ELECTRICAL CONDUCTION IN LI-DOPED NIO [J].
BOSMAN, AJ ;
CREVECOEUR, C .
PHYSICAL REVIEW, 1966, 144 (02) :763-+
[2]  
Carlson D. E., 1979, Amorphous semiconductors, P287
[3]  
CARLSON DE, 1976, APPL PHYS, V28, P617
[4]  
FISTUL VI, 1969, HEAVILY DOPED SEMICO, P143
[5]  
Frenkel J, 1938, PHYS REV, V54, P647, DOI 10.1103/PhysRev.54.647
[6]   High electric field photocurrent of Vidicon and diode devices using wide band gap a-Si:H prepared with intentional control of silicon network by chemical annealing [J].
Futako, W ;
Sugawara, T ;
Kamiya, T ;
Shimizu, I .
JOURNAL OF ORGANOMETALLIC CHEMISTRY, 2000, 611 (1-2) :525-530
[7]   Analytical derivation of the effective temperature for field-dependent hopping conductivity [J].
Godet, C .
PHILOSOPHICAL MAGAZINE LETTERS, 2003, 83 (11) :691-698
[8]   Physics of bandtail hopping in disordered carbons [J].
Godet, C .
DIAMOND AND RELATED MATERIALS, 2003, 12 (02) :159-165
[9]   Variable range hopping revisited: the case of an exponential distribution of localized states [J].
Godet, C .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2002, 299 :333-338
[10]  
Hosono H, 1996, J NON-CRYST SOLIDS, V200, P165, DOI 10.1016/0022-3093(96)80019-6